In the following, we check four measured processes \(e^+e^-\rightarrow K_2^{*0}(1430)K^-\pi ^+\)  [1]}, \(e^+e^-\rightarrow \phi \pi ^+\pi ^-\)  [2]}, \(e^+e^-\rightarrow \phi f_0(980)\)  [2]}, and \(e^+e^-\rightarrow \phi f_2(1525)\)  [1]}. For \(e^+e^-\rightarrow K_2^{*0}(1430)K^-\pi ^+\) , there exist abundant event clusters. Since these predicted higher \(\rho \) , \(\omega \)  and \(\phi \)  states can decay into open-strange meson pair, it is difficult to distinguish \(\rho \) , \(\omega \)  and \(\phi \)  states via the \(e^+e^-\rightarrow K_2^{*0}(1430)K^-\pi ^+\)  channel. Further data analysis of \(e^+e^-\rightarrow K_2^{*0}(1430)K^-\pi ^+\)  is an interesting research issue similar to the way adopted in Refs. [5]}, [6]}.
